Method for determining tribological properties of a sample surface using a scanning microscope (sem) and associated scanning microscope

ABSTRACT

Described is a method for examining a surface of a sample using an atomic force scanning microscope (AFM) comprising a cantilever with a longitudinal extension along which a measuring tip is disposed, which is selectively arranged relative to said sample surface by a driver means and whose spatial position is detected using a sensor unit, and said microscope is provided with at least one ultrasound generator, which initiates vibration excitation at a given excitation frequency between said sample surface and said cantilever, the measuring tip of which is brought into contact with said sample surface in such a manner that said measuring tip is excited to vibrations which are oriented lateral to said sample surface and perpendicular to said longitudinal extension of said cantilever and that the torsional vibrations induced in said cantilever are detected and analyzed by means of an evaluation unit. The invention is distinguished in that the vibration excitation occurs in such a manner that the oscillations executed by the measuring tip have higher harmonic vibration parts relative to the excitation frequency, that vibration excitation is conducted at excitation amplitudes which lead inside the cantilever to torsional amplitudes, the maximum values of which form a largely constant plateau value despite increasing excitation amplitudes and the resonance spectra of which undergo, in the range of the maximum values of the torsional amplitudes, a widening of the resonance spectrum which is determinable by a plateau width, and that used for examining the sample surface are the resonance spectra, preferably the plateau value, the plateau width and/or the gradient of the respective resonance spectra.

TECHNICAL FIELD

The present invention relates to a method for examining a sample surface using an atomic force scanning microscope comprising a cantilever with a longitudinal extension, along which the measuring tip is arranged precisely relative to a sample surface by means of a driver means, the spatial position of the measuring tip being determined by a sensor unit. The microscope is further provided with at least one ultrasound generator with which vibration excitation is initiated at a given excitation frequency between the sample surface and the cantilever, the measuring tip thereof is brought in contact with the sample surface in such a manner that the oscillations imparted to the measuring tip are oriented lateral to the sample surface and perpendicular to the length of the cantilever. The torsional vibrations induced in the cantilever are detected and analyzed by means of an evaluation unit.

PRIOR ART

The development of an atomic force scanning microscope has permitted major achievements in the field of examination of surface properties, in particular in the characterization of surface properties. For the first time, it is possible to obtain information concerning surfaces and areas close to the surface of very different samples in nanometer resolution even in the magnitude of single atoms. Friction force microscopy, a further development of the atomic force scanning microscope, permitted for the first time studying one of the oldest problems in science, the examination of friction, on this scale.

DE 43 24 983 C2 describes an acoustical microscope operating on the technological basis of an atomic force scanning microscope that is able to measure the topography as well as the elastic properties of the surface of a sample. The microscope comprises a cantilever designed as a leaf spring, usually with a length of between 100 μm and 500 μm, attached to the one end of which is a pyramid-shaped measuring tip having a tip radius of curvature of about 50 nanometers.

In order to measure and examine the sample surface holistically, the cantilever and the measuring tip attached thereto are scanned over the sample surface with the aid of a suited moving means in such a manner that the measuring tip makes contact with the sample surface with a given vertical load at every single scanning point. The optical sensor unit permits determining the degree of deformation of the cantilever and thus the topography-based excursion of the measuring tip. Usually, the optical sensor unit is provided with a laser diode from which a laser beam directed at the cantilever is emitted, reflected thereat, and detected by a position-sensitive photodiode. During scanning, the cantilever and the measuring tip are guided perpendicular to the sample surface via a regulation loop in such an active manner that the excursion of the cantilever, respectively the vertical load with which the cantilever lies on the sample surface via the measuring tip, remains constant. The regulation tension required for the excursion is usually converted into a distance value and is correspondingly depicted encoded as a color value in a representation showing the surface topography.

In order to also be able to determine the elastic properties of the surface sample, an ultrasound generator is provided which induces oscillations in the surface sample while the measuring tip lies at a scanning point of the sample surface. Vibration excitation by coupling in ultrasonic waves leads to normal vibrations of the sample surface which induce high-frequency oscillating bending vibrations in the cantilever along its longitudinal extension.

Detection by the ultrasonically induced, high-frequency vibration behavior of the cantilever permits obtaining information about the elastic properties of the sample surface. The problem with this measuring situation that needs to be resolved lies in the decoupling due to the measurement of the superimposed excursions of the cantilever, which stem, on the one hand, from the topography measurement due to which the vertical load with which the measuring tip lies on the sample surface remains, as constant as possible and, on the other hand, which cause the ultrasonically induced normal vibrations of the sample surface transmitted to the cantilever via the measuring tip.

In order to obtain a reliable measuring signal with a high as possible signal/noise ratio for measuring the elasticity, the ultrasonically induced vibration excitation of the sample surface occurs at frequencies which are at least one magnitude greater than the resonant frequency of the cantilever having the measuring tip attached thereto. Using two photodiodes with different temporal responding behavior, on which the light beam reflected at the cantilever impinges, permits selective detection and evaluation of the vibration behavior of the cantilever. Thus the photodiode with a slow response behavior is able to solely detect the excursions stemming from the contour-based readjustment of the cantilever for determining the topography. On the other hand, the second photodiode, which has a bandwidth window in the MHz range, is provided for determining the high-frequency vibration parts of the cantilever. Especially suited therefor are, for example, single-cell light-sensitive detectors with a smooth-edged shading means, for example in the form of a razor blade or a so-called heterodyne running-time interferometer, in the one interferometer arm of which a frequency shift means is provided. Such a type rapid responding detection unit can also be designed based on a capacity measurement, in which the measuring capacity is formed from the cantilever and a needle-shaped counter-electrode disposed opposite thereto. Further details can be found in the aforementioned printed publication DE 43 24 983 C2.

Contrary to the aforedescribed resonance measurement with vertical modulation, i.e. the to-be-examined sample surface is excited to normal vibrations, U.S. Pat. No. 5,804,708, describes an atomic force microscope with a similar setup, but vibration excitation of the to-be-examined sample occurs with the aid of a signal generator in such a manner that the sample surface imparts vibrations oriented lateral to the sample surface and, in particular, directed transverse in relation to the longitudinal extension of the cantilever.

The vibration excitation directed transverse to the longitudinal extension of the cantilever induces torsional vibrations in the cantilever in contact with the sample surface via the measuring tip, with the measuring tip, which is at least sometimes in contact with the sample surface, executing oscillations which are directed in longitudinal direction to the sample surface and transverse to the longitudinal extension of the cantilever, respectively are polarized. The measuring tip briefly adheres to the sample surface at the point of reversal of the oscillations. The sample surface is deformed by the shear forces acting laterally to the sample surface until, due to friction, the measuring tip slips out of the described state back over the sample surface.

The shear deformations formed at the returning points in dependence on the vertical load with which the measuring tip lies on the sample surface influence the vibration behavior of the measuring tip and consequently that of the cantilever in a manner which characterizes the elastic properties of the sample surface. Thus it is possible to obtain information about the elastic properties of the sample surface from the vibration behavior, for example from the vibration amplitude and/or the phase of the oscillations occurring in the form of torsional vibrations along the cantilever.

The oscillations initiated by the signal generator in the sample have frequencies of approximately 1 kHz. However, with this measuring method, local resolution has proven unsatisfactory. Only measurements with a local resolution of approximately 100 nm can be achieved. Moreover, the measuring quality achievable with this method permits obtaining only qualitative information about the frictional properties of the sample surface.

DESCRIPTION OF THE INVENTION

The object of the present invention is to further develop a method for examining a surface sample using an atomic force scanning microscope of the aforedescribed manner, in which vibrations are induced in the surface sample, the vibrations being directed lateral to the sample surface and, moreover, being oriented perpendicular to the longitudinal extension of the cantilever, in such a manner that it is possible to obtain qualitative and quantitative information about the frictional properties of the sample surface. In particular, the object is to permit high locally resolved determination of the tribological, i.e. frictional properties of the sample surface, by means of superimposing a topography measurement, permitting in this manner finely as possibly resolved sample surface mapping with a local resolution of less than 100 nm, preferably less than 10 nm.

The solution to the object of the present invention is set forth in claim 1. Advantageous features that further develop the invented method are the subject matter of the subordinate claims and of the description with reference to the preferred embodiments.

A key element of the present invention is that a method for examining a sample surface by means of an atomic force scanning microscope comprising a cantilever with a longitudinal extension, along which a measuring tip is disposed, which is selectively arranged relative to the sample surface via a driver means and the spatial position of which is detected by a sensor unit, and is provided with at least one ultrasound generator, which initiates a vibration excitation with a given excitation frequency between the sample surface and the cantilever, the measuring tip thereof is brought into contact with the sample surface, in such a manner that the vibrations imparted to the measuring tip are oriented lateral to the sample surface and perpendicular to the longitudinal extension of the cantilever and that torsional vibrations forming in the cantilever are detected and analyzed by means of an evaluation unit, is distinguished in that vibration excitation occurs in such a manner that the oscillations executed by the measuring tip have higher harmonic vibration parts relative to the excitation frequency. The vibration excitation preferably occurs with a continuous wave signal which is wobbled, i.e. varied, within a given excitation frequency range. The excitation frequency range is selected in such a manner that the resonant basic vibration of the cantilever having the measuring tip in contact on the sample surface lies inside the excitation frequency range.

In addition to the selection of a suited frequency, vibration excitation of the cantilever lying on the sample surface occurs with excitation amplitudes leading in the cantilever to torsional vibrations with torsional amplitudes whose torsional amplitude maximum values assume a largely constant plateau value despite increasing excitation amplitudes and whose resonance spectra undergo in the range of the torsional amplitude maximum value a widening of the resonance spectrum which is determinable by the width of the plateau. Finally, the resonance spectra, preferably the plateau value, the plateau width, the gradient of the respective resonance spectra at the flanks of the resonance curve and/or the gradient of the plateau can be utilized to examine the sample surface.

With the aid of the invented method, tribological properties, thus for example the frictional forces or the frictional coefficients acting between the measuring tip and the sample surface are detected at the sample surface with a local resolution of up to 1 nm. Compared to prior art methods, which at best permit local resolution of approximately 100 nm, the invented method is a highly sensitive and most finely resolving tribological method of analysis. In addition to determining tribological properties at a sample surface, the invented method, of course, also permits determination of the topography by adjusting a constant vertical load with which the measuring tip of the cantilever lies on the to-be-examined sample surface. With the aid of a detection means, low-frequency excursions of the measuring tip are detected via the reflection of light at the cantilever and correspondingly evaluated. The detection signal obtained with the aid of the detection means representing the low-frequency topography-based excursion of the measuring tip serves, on the one hand, to determine the topography and, on the other hand, as a regulation value, with which the distance between the measuring tip and the sample surface, respectively the vertical load with which the measuring tip lies on the sample surface is held constant temporally averaged. In this manner, the invented method permits rendering in successive scanning of the surface an accurate microscopic topographic image of the sample surface in a scale of up to 1 nm, the image being able at the same time to provide tribological information about the sample surface.

Measurement of tribological surface properties at a point of the sample surface preferably occurs in several steps. First, for determining the basic resonant frequency of the cantilever in contact with the sample surface via the measuring tip, the ultrasound generator generates vibrations in the form of continuos wave signals whose frequencies are wobbled, i.e. varied, in a given frequency range. The given frequency comprises preferably frequencies below the basic resonant frequency range of the cantilever in contact with the sample surface via the measuring tip up to thirty times this contact resonant frequency. Typically, frequency wobbling of the excitation frequency occurs in 1 kHz frequency steps within a frequency range between 50 kHz and 10 MHz. For example, in the case of a typical cantilever with a length of 450 μm, there were four torsional resonances in the frequency range between 50 kHz and 3 MHz.

In order to determine the properties of the sample surface, in particular with regard to the tribological properties such as frictional coefficients etc., the sample is impinged via the ultrasound generator with excitation frequencies lying in the contact resonant frequency f_(r). Preferably, the excitation frequency range comprises Δf_(a) frequencies from f_(r)−½f_(r) to f_(r)+½f_(r). In a particularly advantageous manner, the excitation frequency range Δf_(a) comprises frequencies between f_(r)−½Δf_(r) to f_(r)+½Δf_(r), with Δf_(r) corresponding to the half-width value of the determined resonance curve measured at f_(r).

Vibration excitation occurs within the framework of a frequency sweep, i.e. the excitation frequency is wobbled, respectively varied, in the given excitation frequency range Δf_(a) in the form of single continuous wave signals.

In addition to selecting the excitation frequency range in the range of the contact resonant frequency, of utmost relevance is the exact setting of the direction of the vibrations, respectively of the polarization of the vibration of the transverse vibrations induced laterally in the sample surface relative to the longitudinal extension of the cantilever. Setting the measuring tip lying on the sample surface with a defined vertical load results in high-frequency oscillating transverse vibrations transverse to the longitudinal extension of the cantilever which due to the great rise in resonant vibrations constantly “jumps back and forth” between the following three states: 1) the measuring tip rubs over the sample surface; 2) oscillation movement comes to a standstill; 3) the measuring tip moves within an elastic potential, i.e. the measuring tip briefly engages in a frictional bond with the sample surface, locally deforming the sample surface due to the shear forces directed lateral thereto.

In contrast to the non-resonant case, as described in U.S. Pat. No. 5,804,708, in which the measuring tip executes strict cyclical oscillations with the measuring tip, in the resonant vibration case, the measuring tip dances at least sectionwise chaotically over the sample surface and assumes the aforedescribed states stochastically. This is referred to as “stick-slip” motion. This motion represents a highly dynamic motion behavior.

Due to the measuring situation described in the preceding, it is not difficult to understand that the vibration behavior forming inside the cantilever is determined by the tribological contact properties between the measuring tip and the sample surface. If the sample surface is excited, as mentioned in the preceding, with a contact resonant frequency, preferably the basic resonant frequency of the cantilever in contact with the sample surface via the measuring tip to vibrations by means of the ultrasound generator, at low excitation amplitudes, resonant vibration behavior of the cantilever sets in, the resonance curve of which is largely symmetrical. The resonant vibration behavior of the cantilever is detected in a prior art manner by means of an optical sensor unit and represented in the form of a resonance curve. If the excitation amplitude is raised by successively increasing the excitation voltage with which the ultrasonic wave generator is operated, the recorded resonance spectrum shows deviations from the originally symmetrical resonance curve of such a manner that, despite increasing excitation amplitude, the amplitude of the resonance spectrum assumes a type of saturation value and remains practically constant. Similarly, the form of the resonance curve changes in such a manner that a widening is generated in the upper amplitude range or the resonance curve. Along with the widening of the resonance spectrum of the resonance curve, a sort of plateau forms, whose position remains largely constant despite rising excitation amplitudes, the width of which however also increases with rising excitation amplitudes. According to the invention, it is these characteristic deviations from the symmetric formation of the resonance curve formed by the increase in excitation amplitude that are selectively used to obtain tribological information. This particularly applies to the plateau values, the plateau width, the gradient of the respective resonance spectra at the flanks of the resonance curve and/or the gradient of the plateau yielded by a widening of the resonance spectrum.

The aforedescribed resonant excitation can, of course, also be carried out at contact resonant frequencies of a higher order. Thus, the aforedescribed deviations from the symmetric formation of the resonance curve can be observed not only at the basic resonant frequency, that is in the occurrence of the first torsion mode, but also at higher modes. The widening occurring in the resonance curve at higher modes, such as in the plateau width, can also be utilized for determining the frictional force.

In addition, “overtones” to the excitation frequency can be detected in the resonant behavior of the cantilever as soon as the described flattening at the resonance maximum sets in. Such type overtones can also be detected at higher vibration modes, which also can be utilized to determine the frictional force. For example, if a cantilever in contact with the surface has the first torsion mode at an excitation frequency of 100 kHz, the higher torsion modes lie at 300 kHz, 500 kHz, 700 kHz, etc. The n^(th) torsion mode, therefore, lies at (2n−1)×100 kHz. If the first torsion mode is excited with a sufficiently high excitation amplitude so that, for example, a flattened torsion peak is visible in the excitation frequency spectrum between 80 kHz and 120 kHz, peaks occur as well at 200 kHz, 300 kHz, 400 kHz, etc., also at frequencies k×100 kHz, which are singly detectable. The overtones of the excitation frequency that coincide with higher torsion modes (300 kHz, 500 kHz, 700 kHz, . . . ) are, of course, more intensive than the others (200 kHz, 400 kHz, 600 kHz, . . . ).

For detection of the resonant torsional vibrations forming inside the cantilever, at least one temporally high-resolving photodiode is used, whose temporal resolution capacity permits detection of the vibration occurrences with frequencies, which preferably correspond to up to twenty-five times, preferably double to ten times the excitation frequency.

By means of the sequential scanning in the measuring tip along the sample surface, measurements are conducted successively at closely adjacent contact points spaced laterally at least approximately 1 nm under the aforedescribed resonance conditions. On the one hand, the measurements yield information about the surface topography as well as, on the other hand, about the tribological properties at the point of contact. In addition to the topographically determined surface contour, the aforementioned properties of the resonance curve of the cantilever at each point of the to-be-measured sample surface can be plotted and encoded as a color value for representation. For example, changing frictional properties at the sample surface influence the resonant vibration behavior of the cantilever and therefore the vibration amplitude at constant excitation frequency making even the smallest changes in friction detectable as it is these smallest changes in friction that have very sensitive influence on the amplitude behavior, as is clearly indicated by the recorded resonance curves.

For example, the smallest shifting of the flanks of the resonance curve in relation to the frequency axis (x-axis) results in major changes in the resonance amplitude (y-axis). As already mentioned, besides detecting the resonant behavior of the basic vibration of the cantilever, higher harmonic resonances can also be detected and examined and correspondingly encoded as a color value for representation.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention is made more apparent in the following using preferred embodiments with reference to the accompanying drawings, by way of example, without intention of limiting the scope or spirit of the inventive idea.

FIG. 1 shows a schematic representation of components for conducting the invented method, and

FIG. 2 shows a diagrammatic representation with resonance curves at different excitation amplitudes.

WAYS TO CARRY OUT THE INVENTION, COMMERCIAL APPLICABILITY

FIG. 1 shows an atomic force scanning microscope for conducting the invented method for examining a sample surface, in particular for determining tribological properties on the sample surface. The microscope depicted in FIG. 1 is provided with a cantilever 1, whose measuring tip 2 lies on the sample surface 3 of a sample P. Sample P is in contact with an ultrasonic transducer 5 via a pre-run track or pre-run layer 4. The ultrasonic transducer 5 is set into oscillations by a corresponding signal generator 6. The pre-run layer 4 is, for example, connected on both sides to the sample P and the ultrasonic transducer via a honey layer as an acoustic coupling layer.

An optical sensor unit comprising a laser diode 7, a deflection mirror 8 and a photodiode unit 9, is provided for measuring the vibrations conveyed into the cantilever 1 via the measuring tip 2. The photodiode unit 9 serves, on the one hand, to detect the topographically based, low-frequency excursions of the measuring tip 2 and therewith of the cantilever and, for this reason, is connected to an AFM back-coupling loop 10, which serves to constantly adjust the vertical load with which the measuring tip 2 lies on the sample surface 3. Details concerning such a type control loop are described in the printed publication DE 43 24 983 C2 described in the introductory part hereof.

Similarly, the photodiode unit 9 is able to detect high-frequency vibration parts which are conveyed as a torsional signal T to a computing unit 12 via a rapid signal processing unit 11, stored, evaluated and finally graphically represented as frictional properties.

For reason of clarity, the friction microscope setup shown quite schematically in FIG. 1 does not show the driver means required for the spatial arrangement of the cantilever relative to the sample surface, usually provided as a piezo driver means. As it is a state-of-the-art driver means, here too reference is made to DE 43 24 983 C2.

In order to carry out the examination on sample P according to the present invention, the object of which is measuring the tribological properties at sample surface 3, the ultrasonic transducer 5 is designed and operated in such manner that sample P is set in vibrations solely lateral to the sample surface 3. The vibrations are, in addition, oriented perpendicular to the longitudinal extension of the cantilever 1, respectively are polarized (see arrow in FIG. 1). The mechanical coupling sets the cantilever 1 in contact with the sample surface 3 via the measuring tip 2 in torsional vibrations, which upon reaching a basic resonant frequency lead to a great rise in torsional resonance vibration. For selective determination of the basic resonant frequency f_(r) of the cantilever 1 in contact with the sample surface 3 via the measuring tip 2, the ultrasound generator 5, which is composed of the vibration generator 6 and the ultrasonic transducer 5, generates a multiplicity of continuous wave signals separated in temporal succession, whose excitation frequencies are wobbled in a given frequency range, including frequencies below the basic resonant frequency of the cantilever up to thirty times this frequency, thereby ensuring that cantilever 1 is excited to torsional vibrations not only with its basic vibration but also begins vibrating at higher mode torsional resonances. Upon reaching a contact resonant frequency, either the basic resonant frequency or a higher harmonic resonant frequency, the excitation amplitude, with which the ultrasonic transducer 5 vibrates, is set in such a manner that measuring tip 2 rubs on the sample surface 3, thus always changing the elastic contact to the sample surface. In detail, at these excitation amplitudes, the measuring tip 2 carries out oscillating sliding movements which are briefly interrupted at the point of reversal of the oscillation by friction bonding between the measuring tip 2 and the sample surface 3.

The resonance behavior of the cantilever 1 setting in with this vibration behavior, also described as “stick-slip” vibration behavior, is detected by an optical sensor unit 9 and analyzed more exactly by way of a resonance curve representation. A family of curves obtained with the aid of the measuring setup described in FIG. 1 is depicted in a diagram shown in FIG. 2, which provides an abscissa formed as a frequency axis and an ordinate formed as an amplitude axis. The resonance curves depicted with the different sorts of lines represent the resonance behavior of the cantilever at different excitation amplitudes, respectively excitation voltages. It appears that at low vibration amplitudes of the ultrasonic transducer, the amplitudes of the respective resonance maximum values increase linearly with the amplitude of the excitation vibration. At excitation voltages of approximately up to 3 to 4V, largely symmetrical resonance curves form. From a certain excitation amplitude, respectively excitation voltage, the amplitudes of the resonance curves, respectively of the torsion resonances, remain largely constant despite rising excitation voltages, but rather the shape of the resonance curve changes. The reason for such type nonlinear changes in the shape of the resonance curve is found in the aforedescribed “stick-slip” behavior. If however the excitation amplitude is raised nonetheless, the diagram shows that the position of the torsional resonance remains largely the same and a widening of the spectrum in the form of a plateau occurs in the range of the torsional maximum. It is these curve-changing characteristics that are utilized according to the present invention to determine the frictional properties, respectively the tribological properties, of the sample surface. This relates, in particular, to the plateau value of the resonance amplitudes, the plateau widths and the gradient of the resonance curve flanks forming a saturation value.

The evaluation of the resonant torsional vibration behavior of the cantilever occurs by means of recording the phase distribution and frequency distribution of the torsional vibrations of the cantilever by way of optical determination of vibrations including using a lock-in amplifier. An alternative to the lock-in amplifier is using a wideband amplifier in conjunction with discrete signal processing for spectral analyses, such as for example the discrete Fourier transformation (DFT), the rapid Fourier transformation (FFT), the wavelet transformations, or the so-called Walsh transformation. Analogue spectral analysis is also feasible.

LIST OF REFERENCE

-   1 cantilever -   2 measuring tip -   3 sample surface -   4 pre-run layer -   5 ultrasonic transducer -   6 signal generator -   7 laser diode -   8 deflection mirror -   9 photodiode unit -   10 AFM back coupling loop -   11 rapid signal processing unit -   12 computing unit -   P sample -   T torsional signal -   f excitation frequency -   A amplitude 

1. A method for examining a surface of a sample using an atomic force scanning microscope (AFM) comprising a cantilever with a longitudinal extension along which a measuring tip is disposed, which is selectively arranged relative to said sample surface by a driver means and whose spatial position is detected using a sensor unit, and said microscope is provided with at least one ultrasound generator, which initiates vibration excitation at a given excitation frequency between said sample surface and said cantilever, the measuring tip of which is brought into contact with said sample surface in such a manner that said measuring tip is excited to vibrations which are oriented lateral to said sample surface and perpendicular to said longitudinal extension of said cantilever and that the torsional vibrations induced in said cantilever are detected and analyzed by means of an evaluation unit, wherein said vibration excitation occurs in such a manner that the oscillations executed by said measuring tip have higher harmonic vibration parts relative to the excitation frequency, said vibration excitation is conducted at excitation amplitudes which lead inside said cantilever to torsional amplitudes, the maximum values of which form a largely constant plateau value despite increasing excitation amplitudes and the resonance spectra of which undergo, in the range of said maximum values of said torsional amplitudes, a widening of the resonance spectrum which is determinable by a plateau width, and used for examining said sample surface are said resonance spectra, preferably the plateau value, the plateau width and/or the gradient of the respective resonance spectra.
 2. The method according to claim 1, wherein by way of sequential scanning at a multiplicity of different points of contact between said measuring tip and said sample surface successive resonance spectra are detected and analyzed.
 3. The method according to claim 1, wherein in examining said sample surface, tribological properties such as frictional force and/or frictional coefficients at said sample surface are analyzed and qualitatively and/or quantitatively determined.
 4. The method according to claim 1, wherein said measuring tip makes contact on said sample surface with a vertical load which is constantly adjusted by said driver means.
 5. The method according to claim 1, wherein said ultrasound generator emits a continuous wave signal vibrating at said given excitation frequency, said continuous wave signal being varied by means of frequency wobbulation within a given excitation frequency range Δf_(a).
 6. The method according to claim 5, wherein said given excitation frequency range Δf_(a) is selected in such a manner that the basic resonant vibration f_(r) of said cantilever in contact with said sample surface via said measuring tip is contained within said frequency range.
 7. The method according to claim 6, wherein for determining the basic resonant vibration f_(r) of said cantilever lying on said sample surface with said measuring tip, said sample surface is impinged with a frequency sweep.
 8. The method according to claim 7, wherein said frequency sweep comprises the following frequencies f: f<f _(r) and f<30×f _(r).
 9. The method according to claim 5, wherein said excitation frequency range Δf_(a) comprises frequencies from f_(r)−½f_(r) to f_(r)+½f_(r), preferably f_(r)−½Δf_(r) to f_(r)+½Δf_(r), with Δf_(r) corresponding to the half-width value of the resonance curve at f_(r).
 10. The method according to claim 5, wherein said torsional vibrations of said cantilever lying on said sample surface with said measuring tip are detected using said sensor unit at a frequency range n×Δf_(a), with n<25, preferably 2<n<10.
 11. The method according to claim 2, wherein the information obtainable from said resonance curve at each point of contact between said measuring tip and said sample surface, such as the half-width value Δf_(r) of said resonance curve at f_(r), the plateau width, the plateau value, the gradient at said plateau or the vibration amplitude of the higher harmonics are recorded and represented encoded as color values.
 12. The method according to claim 1, wherein said vibration excitation of said sample surface occurs via said ultrasound generator in such a manner that said ultrasound generator is directly or indirectly acoustically connected with said sample surface.
 13. The method according to claim 1, wherein a microscopic image of said sample surface is obtained by means of sequentially scanning said sample surface, said microscopic image containing information relating to the surface topography as well as the tribological properties.
 14. The method according to claim 1, wherein said torsional vibrations forming inside said cantilever are detected by said sensor unit and the sensor signals obtained by said sensor unit are examined with the aid of a wideband amplifier and subsequent spectral analysis.
 15. The method according to claim 14, wherein said spectral analysis is conducted using numerical Fourier transformation or FFT, Wavelet-transformation or Walsh-transformation. 